Fig 5.75. A passive-grid 400W linear HF
amplifier, the PAOFRI Frinear. Screen-grid voltage is derived from the RF input and no grid bias supply is required

PAOFRI's Frinear-400 is shown in Fig 5.75 [29]. It has several interesting
features.

• Being a passive-grid
amplifier, most of the input power is dissipated in a hefty carbon resistor. The voltage across it is applied to the control-grids of the valves
and, considering the low value of the resistor (50 or 68 Ohm), one might expect this arrangement to be
frequency-independent; however, the capacitances of the four grids, sockets and associated wiring add up to about 100pF which is only 55 Ohm at 29MHz! This capacitance must be tuned out if what is adequate drive on 3.5MHz is to produce full output on the higher-frequency
bands. PAOFRI does this with a dual-resonant circuit (L3 and ganged tuning
capacitors) similar to the well-known E-Z-Match antenna tuner; it covers 3.5-29MHz without
switching.

• The screen grids in this amplifier are neither at a fixed high voltage nor at earth potential but at a voltage which is proportional to the RF
drive. To that end, the RF input is transformed up 3: 1 in T1, rectified in a voltage doubler and applied to the four bypassed screen grids through individual
resistors. This method is consistent with good linearity.

• Control-grid bias is not taken from a mains-derived negative supply voltage but the desired
effect, reducing the standing current to 20-25 mA per valve, is obtained by raising the cathodes above earth
potential. The bias voltage is developed by passing each cathode current through an individual 100 Ohm resistor and the combined currents through as many forward-biased rectifier diodes as are required to achieve a total standing current of 80-100mA. The individual cathode resistors help in equalising the currents in the four
valves. During non-transmit periods the third contact set (RLA3) on the antenna changeover relay opens and inserts a large
(10 kOhm) resistor into the combined cathode current, which thereby is reduced to a very low
value.

• The pi-filter coil for 3.5 and 7MHz is wound on a powdered-iron toroid which is much smaller than the usual air-core
coil. This is not often seen in high-powered amplifiers due to the fear that the large circulating current might saturate the core and spoil the intermodulation performance but no distortion was discernible in a two-tone
test.

• In Fig5.75, the 42V filaments of the four valves and a capacitor are
shown series connected to the 240V mains. This 0.3A chain is the way these valves were intended to be used in CTV sets and it does save a filament
transformer, but this method is not recommended for experimental apparatus such as a home construction
project. Besides, a 6u.F 250VAC capacitor is neither small nor inexpensive, and generally not available from component
suppliers. Also, with lethal mains voltage in the amplifier chassis, the mains plug must be pulled every time access to the chassis is required and after the change or adjustment is made there is the waiting for filaments to heat up before applying HT
again. It is much safer and more convenient to operate the filaments in parallel on a 42V transformer (3 x 12.6+ 5V will
do), or to use EL519 valves in parallel, series-parallel or series on 6.3, 12.6 or 25.2V
respectively.